{"id":566,"date":"2017-05-11T17:16:31","date_gmt":"2017-05-11T09:16:31","guid":{"rendered":"http:\/\/yrwu-wk.ee.ntu.edu.tw\/?p=566"},"modified":"2019-02-11T17:24:53","modified_gmt":"2019-02-11T09:24:53","slug":"a-serious-of-3d-random-indium-fluctuation-modeling-with-self-consistent-landscape-theory-has-been-in-physical-review-b","status":"publish","type":"post","link":"https:\/\/yrwu-wk.ee.ntu.edu.tw\/index.php\/2017\/05\/11\/a-serious-of-3d-random-indium-fluctuation-modeling-with-self-consistent-landscape-theory-has-been-in-physical-review-b\/","title":{"rendered":"A serious of 3D Random Indium Fluctuation Modeling with self-consistent landscape theory has been in Physical Review B"},"content":{"rendered":"<ul>\n<li><a href=\"http:\/\/dx.doi.org\/10.1103\/PhysRevB.95.144206\">DOI: 10.1103\/PhysRevB.95.144206<\/a><\/li>\n<li><a href=\"http:\/\/dx.doi.org10.1103\/PhysRevB.95.144205\">DOI: 10.1103\/PhysRevB.95.144205<\/a><\/li>\n<li><a href=\"http:\/\/dx.doi.org\/10.1103\/PhysRevB.95.144204\">DOI: 10.1103\/PhysRevB.95.144204<\/a><\/li>\n<\/ul>\n\n\n<p><em>Chi-Kang Li, Marco Piccardo, Li-Shuo Lu, Svitlana Mayboroda, Lucio Martinelli, Claude Weisbuch, Marcel Filoche, Yuh-Renn Wu*, <\/em>    \u201cLocalization landscape theory of disorder in semiconductors III:    Application to transport and radiative recombination in light emitting    diodes.\u201d, Phys. Rev. B, 95, 144206 , April, 2017. <\/p>\n\n\n\n<p><em>Marco  Piccardo, Chi-Kang Li, Yuh-Renn Wu, James  S. Speck, Bastien Bonef,   Bob Farrell, Marcel Filoche, Lucio Martinelli,  Jacques Peretti, and  Claude Weisbuch, <\/em>\u201cLocalization landscape  theory of disorder in  semiconductors II: Urbach tails of disordered  quantum well layer\u201d,  Phys. Rev. B, 95, 144205, April, 2017. <\/p>\n\n\n\n<p><em>Marcel Filoche, Marco Piccardo, Yuh-Renn Wu, Chi-Kang Li, Claude Weisbuch, and Svitlana Mayboroda, <\/em>\u201c Localization landscape theory of disorder in semiconductors I: Theory and modeling\u201d, Phys. Rev. B, 95, 144204, April, 2017. <\/p>\n","protected":false},"excerpt":{"rendered":"<p>DOI: 10.1103\/PhysRevB.95.14420&#8230; <\/p>\n","protected":false},"author":1,"featured_media":572,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[],"class_list":["post-566","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-uncategorized"],"_links":{"self":[{"href":"https:\/\/yrwu-wk.ee.ntu.edu.tw\/index.php\/wp-json\/wp\/v2\/posts\/566","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/yrwu-wk.ee.ntu.edu.tw\/index.php\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/yrwu-wk.ee.ntu.edu.tw\/index.php\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/yrwu-wk.ee.ntu.edu.tw\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/yrwu-wk.ee.ntu.edu.tw\/index.php\/wp-json\/wp\/v2\/comments?post=566"}],"version-history":[{"count":3,"href":"https:\/\/yrwu-wk.ee.ntu.edu.tw\/index.php\/wp-json\/wp\/v2\/posts\/566\/revisions"}],"predecessor-version":[{"id":573,"href":"https:\/\/yrwu-wk.ee.ntu.edu.tw\/index.php\/wp-json\/wp\/v2\/posts\/566\/revisions\/573"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/yrwu-wk.ee.ntu.edu.tw\/index.php\/wp-json\/wp\/v2\/media\/572"}],"wp:attachment":[{"href":"https:\/\/yrwu-wk.ee.ntu.edu.tw\/index.php\/wp-json\/wp\/v2\/media?parent=566"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/yrwu-wk.ee.ntu.edu.tw\/index.php\/wp-json\/wp\/v2\/categories?post=566"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/yrwu-wk.ee.ntu.edu.tw\/index.php\/wp-json\/wp\/v2\/tags?post=566"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}